WO2004054054A1 - Laser a cavite externe a compensation de dispersion pour accord sans saut de mode - Google Patents

Laser a cavite externe a compensation de dispersion pour accord sans saut de mode Download PDF

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Publication number
WO2004054054A1
WO2004054054A1 PCT/US2003/037440 US0337440W WO2004054054A1 WO 2004054054 A1 WO2004054054 A1 WO 2004054054A1 US 0337440 W US0337440 W US 0337440W WO 2004054054 A1 WO2004054054 A1 WO 2004054054A1
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Prior art keywords
external cavity
light
wavelength
prism
cavity laser
Prior art date
Application number
PCT/US2003/037440
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English (en)
Inventor
Guangzhi G. Zhang
Original Assignee
New Focus, Inc.
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Priority to AU2003295832A priority Critical patent/AU2003295832A1/en
Publication of WO2004054054A1 publication Critical patent/WO2004054054A1/fr

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Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08—Construction or shape of optical resonators or components thereof
    • H01S3/08018—Mode suppression
    • H01S3/08022—Longitudinal modes
    • H01S3/08031—Single-mode emission
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/106—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity
    • H01S3/1062—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating by controlling devices placed within the cavity using a controlled passive interferometer, e.g. a Fabry-Perot etalon
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00—Semiconductor lasers
    • H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
    • H01S5/14—External cavity lasers
    • H01S5/141—External cavity lasers using a wavelength selective device, e.g. a grating or etalon

Definitions

  • the present invention relates generally to external cavity lasers with mechanisms and methods for ensuring mode-hop-free wavelength tuning.
  • Tunable lasers have been developed to address this requirement.
  • tunable external cavity lasers have found wide acceptance in various fields of optics as sources of tunable laser light.
  • External cavity lasers derive their light from a lasing medium positioned within an external cavity typically delimited by two reflectors.
  • the mechanism for tuning the external cavity lasers includes a diffraction grating and a rotatable reflector that selects a desired wavelength from the light diffracted by the grating.
  • the type of external cavity used by this laser is frequently referred to as a Littman cavity and its implementation for wavelength tuning of external cavity lasers have been described in numerous prior art publications, including Michael G. Littman et al., "Spectrally Narrow Pulse Dye Laser Without Beam Expander", Applied Optics, Vol. 17, No. 14, July 15, 1978, pp. 2224-2227.
  • the lasing medium provides gain over a wide wavelength range or tunable range, while the optical path length of the external cavity defines discrete longitudinal modes of light that are supported by the cavity in accordance with the standing wave condition.
  • the light resonating within the external cavity can occupy any of those longitudinal modes provided that the gain of the lasing medium at the corresponding wavelength is sufficiently high.
  • the band delimited by the wavelength selection mechanism covers several adjacent modes, then the light obtained from the external cavity can contain wavelengths defined by these adjacent modes. Clearly, this is not desirable. Consequently, the mechanism for tuning the laser wavelength should be narrow band, i.e., it should define a narrow band containing just one of these longitudinal modes at any wavelength within the tuning range.
  • the tuning should also be effectuated such that at all times the light derived from the cavity remains in one longitudinal mode. Such operation is frequently referred to as continuous single mode scan.
  • a tunable external cavity laser equipped with a medium for emitting a light into the cavity.
  • the laser has an optical path length compensator for adjusting an optical path length of the cavity to thus define a set of longitudinal lasing modes supported by the cavity as dictated by the standing wave condition.
  • the laser also . has a wavelength selector for selecting an operating wavelength of the light in a single longitudinal mode chosen from the set of modes .
  • the laser has a dispersion compensator for compensating a dispersion of the light.
  • a synchronizer is provided for synchronizing the optical path length compensator, the wavelength selector and the dispersion compensator to maintain the light in the selected single longitudinal mode while the wavelength selector tunes the operating wavelength.
  • the optical path length compensator is a prism and the wavelength selector is a wavelength filter, such as a wedge filter.
  • the dispersion compensator uses a pair of prisms and the optical path length compensator uses one of the prisms selected from the pair for optical path length compensation.
  • the second prism of the pair compensates for an angular dispersion and also serves the function of the optical path length compensator.
  • an apex angle ⁇ 2 of the prism used as the optical path length compensator, i.e., of the second prism, is derived from the wedge angle .
  • the synchronizer is a moving stage designed for moving the optical path length compensator, the wavelength selector and the dispersion compensator. It is preferred that the moving stage be driven by a piezo-electric actuator. In the event that a pair of prisms is used as optical path length compensator and dispersion compensator one of the prisms is mounted on the moving stage. Specifically, the prism that is used for adjusting the optical path length is mounted on the stage.
  • the pair of prisms defines a gap filter having a wedge angle .
  • the gap filter forms the wavelength selector and is defined between a first surface of the first prism and a second surface of the second prism of the prism pair.
  • the first and second surfaces are coated with a high reflectivity coating to improve the efficiency of the gap filter.
  • the apex angle Q of the prism used as the path length compensator is derived from the wedge angle of the gap filter.
  • the adjusting of the optical path length the selecting of the operating wavelength and the compensating of dispersion are synchronized.
  • the synchronization is carried out in such a way that compensation of the optical path length changes the set of longitudinal modes in sync with wavelength tuning.
  • dispersion compensation prevents the changes in dispersion occurring in the cavity as a result of optical path length changes and wavelength tuning from causing mode-hops.
  • the steps of adjusting, selecting and compensating are performed by displacing an optical path length compensator, a wavelength selector and a dispersion compensator on a moving stage.
  • the step of dispersion compensation involves compensating for an offset dispersion and an angular dispersion.
  • Fig. 1 is a schematic diagram illustrating a preferred embodiment of a tunable external cavity laser with dispersion compensation.
  • Fig. 2 is a diagram illustrating the mode-hop-free operation of dispersion compensated lasers according to the invention.
  • Fig. 3 is a plan view of a portion of the laser of Fig. 1 illustrating the principles of wavelength tuning.
  • Fig. 4 is a plan view of a portion of the laser of Fig. 1 illustrating the principles of component design.
  • Fig. 5 is a plan view of a portion of an external cavity laser in accordance with another embodiment of the invention.
  • Fig. 6 is a plan view of a portion of an external cavity laser in accordance with yet another embodiment of the invention.
  • Fig. 7 is a schematic diagram of an external cavity laser employing a separate output coupler for deriving output light .
  • Fig. 8 is a schematic diagram of an external cavity laser using a Faraday rotator and polarizing beam splitter for deriving output light .
  • Fig. 9 is a schematic diagram of another external cavity laser in accordance with the invention.
  • Fig. 10 is a schematic diagram of yet another external cavity laser in accordance with the invention.
  • Laser 10 has a medium 12 with a first facet 14 and a second facet 16.
  • Medium 12 can be any suitable active or lasing medium exhibiting gain over a band of wavelengths when pumped by an appropriate pumping mechanism (not shown) .
  • To achieve a wide tuning range medium 12 should provide gain over a wide or broad band of wavelengths.
  • a person skilled in the art will be familiar with the various media and corresponding pumping mechanisms.
  • medium 12 is a solid-state medium such as a semiconductor material which is side pumped by a suitable light source (not shown) or by applying a suitable voltage potential.
  • Second facet 16 of medium 12 is coated with a first reflector 18.
  • First reflector 18 delimits the left side of an external cavity 20.
  • the right side of external cavity 20 is delimited by a second reflector 22.
  • first and second reflectors 18, 22 can have different reflectivities and either one or both of them can be used as an "output coupler" to draw an output light 25 from cavity 20.
  • Cavity 20 has a lens 24 for shaping a light 26 emitted by medium 12. Although a single lens 24 is shown in this embodiment, it will be understood that a number of lenses and other optical elements can be used for appropriately focusing, collimating and otherwise shaping light 26. In order to ensure best operation characteristics, however, the number of optical elements in cavity 20 should be kept to a minimum.
  • Cavity 20 also has a pair of prisms 28 consisting of a first prism 30 and a second prism 32.
  • First prism 30 is oriented to receive light 26 through a surface 34 at normal or nearly normal incidence.
  • Light 26 exits first prism 30 through a surface 36 at which it is refracted and enters second prism 32 through a surface 38 at which it is refracted once again.
  • Prism 32 has a surface 40 through which light 26 exits.
  • a wedge filter 42 is positioned after second prism 32 such that light 26 exiting prism 32 passes through wedge filter 42 before arriving at second reflector 22.
  • Second prism 32 and wedge filter 42 are both mounted on a moving stage 48 driven by a piezo-electric actuator 50.
  • actuator 50 is designed to move stage 48 parallel to second surface 36 of first prism 30 as indicated by arrow S.
  • stage 48 is also designed rotate prism 32 and, in still other cases, an additional actuator (not shown) is provided for rotating prism 30. Slight rotation of both prisms 30, 32 allows the operator to make fine adjustments of an optical path length L opt of cavity 20.
  • a control unit 52 is connected to actuator 50 to control its operation.
  • cavity 20 can support light 26 in a number of longitudinal modes at distinct operating wavelengths dictated by optical path length L opt of cavity 20.
  • optical path length L opt experienced by light 26 is equal to a physical length L of cavity 20.
  • the presence of medium 12, lens 24 prisms 30, 32, and wedge filter 42 through which light 26 passes extends optical path length L opt of cavity 20.
  • the optical path length through medium 12 equals to the physical length through medium 12 multiplied by the refractive index of •medium 12.
  • the optical path length through lens 24 is equal to the physical thickness of lens 24 multiplied by the refractive index of lens 24. The same holds for optical path lengths through prisms 30, 32 and wedge filter 42.
  • optical path length L opt is extended by refraction, e.g., between prisms 30, 32 where light 26 propagates at an angle to the axis of cavity 20, as defined by Snell' s law.
  • the indices of refraction vary slightly as a function of wavelength of light 26, and thus optical path length L opt differs for light 26 depending on its wavelength.
  • optical path length L opt as used herein takes all of these effects into consideration.
  • cavity 20 can support light 26 at an operating wavelength ⁇ op for any integer value of N.
  • the possible operating wavelengths in cavity 20 are contained in a band 44 and correspond to wavelengths of longitudinal modes 46 at which medium 12 provides net gain.
  • the envelope of band 44 indicates the gain available at wavelengths of modes 46.
  • the number of modes 46 will typically be considerably larger than shown in Fig . 1.
  • wedge filter 42 performs the function of a wavelength selector. Specifically, wedge filter 42 is used for selecting operating wavelength ⁇ op of light 26 from among the possible wavelengths of modes 46 contained in band 44. This is done by adjusting the thickness of wedge filter 42 through which light 26 has to travel by moving stage 48 up or down with the aid of actuator 50. In the embodiment shown, operating wavelength is set by wedge filter 42 at ⁇ opl .
  • Fig. 2 indicates a wavelength tuning window or pass band 54 produced by wedge filter 42.
  • Pass band 54 has a width 56 and is initially centered on operating wavelength ⁇ opl within band 44.
  • operating wavelength ⁇ op ⁇ corresponds to mode 46j and is flanked from left and right by modes 46i and 46k.
  • Fig. 3 illustrates prism pair 28 and wedge 42 in more detail.
  • light 26 incident on first prism 30 enters it through surface 34 at normal incidence along the axis of cavity 20, here indicated in dashed and dotted line A.
  • Surface 34 is preferably provided with an anti-reflection coating 58 in order to minimize reflection losses experienced by light 26 at surface 34.
  • first prism 30 The propagation of light 26 inside first prism 30 and its refraction upon exiting through surface 36 are determined by a refractive index nj . and an apex angle ⁇ x of first prism 30.
  • nj refractive index
  • ⁇ x apex angle
  • n 0 is the index of free space
  • ⁇ x is the angle of incidence of light 26 at surface 36
  • ⁇ 2 is the angle of refraction of light 26. It should be noted that for light 26 entering surface 34 at exactly normal incidence or along axis A, angle ⁇ i is equal to apex angle ⁇ i.
  • refractive index n x is dependent on wavelength, i.e.:
  • n x at operating wavelength ⁇ opl and at a second operating wavelength ⁇ op2 to which the operator wishes to tune laser 10 are different, i.e.:
  • the angle of refraction of light 26 at surface 36 will change with operating wavelength.
  • the angle of refraction ⁇ ' 2 is:
  • apex angle ⁇ 2 and refractive index n 2 are equal to those of first prism 30, and surfaces 36, 38 are maintained in parallel.
  • angle of incidence ⁇ i is equal to the angle of refraction experienced by light 26 at surface 36 of first prism 30. This condition holds irrespective of operating wavelength, such • that angle of incidence ⁇ x is equal to ⁇ 2 at operating wavelength ⁇ opl and to ⁇ ' 2 at operating wavelength ⁇ op2 .
  • offset dispersion incurred due to wavelength tuning where the difference in offset dispersion ⁇ od is conveniently referred to as offset dispersion incurred due to wavelength tuning.
  • surface 40 is provided with an anti-reflection coating 60 to minimize reflection losses suffered by light 26 at surface 40.
  • Wedge filter 42 has a taper or wedge angle that is sufficiently small to ensure that wedge filter 42 is efficient in selecting the operating wavelength. In some embodiments, this can be achieved by ensuring that wedge angle is small enough such that wedge filter 42 acts as a Fabry-Perot etalon. This condition will be satisfied when the reflectivities R l r R 2 of surfaces 62, 64 of wedge filter 42 and thickness t of wedge filter 42 along the path of light 26 obey the following etalon approximation: a
  • n w ( ⁇ ) is the wavelength-dependent index of refraction of wedge filter 42
  • wedge filter 42 sets operating wavelength in accordance with the well-known Fabry- Perot etalon principles .
  • Wavelength tuning is achieved by moving wedge filter 42 along the direction parallel to surface 36 such that the thickness t through which light 26 propagates between surfaces 62, 64 is varied, and thus the wavelength passed by etalon 42 is tuned. Precision in this movement is ensured by control 52, which sends an accurately controlled voltage signal to actuator 50 to move stage 48 by a distance ⁇ d in a well-behaved manner.
  • the tuning of operating wavelength effectuated by wavelength selector has to be accompanied by a corresponding adjustment of the optical path length L opt of the external cavity and compensation of angular dispersion.
  • L opt optical path length of the external cavity
  • angular dispersion it is important to provide synchronized optical path length compensation, wavelength selection and dispersion compensation to maintain light in a selected longitudinal mode while the wavelength selector tunes the operating wavelength. This is done to ensure mode-hop-free wavelength tuning of the laser over the available band.
  • wavelength selector represented by wedge filter 42 and path length compensator represented by second prism 32 are mounted on stage 48 and moved in unison to synchronize wavelength selection and optical path length compensation.
  • prism pair 28 represents the dispersion compensator, more specifically, the angular dispersion compensator. Ensuring that surfaces 36 and 38 are maintained in parallel during the movement of stage 48 ensures proper angular dispersion compensation between prisms 30, 32 of prism pair 28. It should be noted that unlike changes in angular dispersion ⁇ ad changes in offset dispersion ⁇ od do not require compensation because they are orthogonal to axis A of cavity 20 and hence do not have any effect on optical path length L opt .
  • apex angle ⁇ 2 of prism 32 has to be in a specific relationship to wedge angle , i.e., apex angle ⁇ 2 of path length compensating prism 32 is derived from wedge angle . It should be noted that in the preferred embodiment apex angles ⁇ x and ⁇ 2 are equal, and hence a derivation of apex angle ⁇ 2 is tantamount to a derivation of both apex angles.
  • Fig. 4 illustrates the derivation of the relationship between wedge angle and apex angle ⁇ 2 for a general case.
  • light 26 at an initial operating wavelength ⁇ 0 is assumed to pass through an optical path length L opt ( ⁇ 0 ) in prism 32 and through a physical thickness t 0 in wedge filter 42.
  • stage 48 produces a displacement of prism 32 and wedge filter 42 by a distance ⁇ d.
  • physical path of light 26 through prism 32 is extended by a length ⁇ l.
  • the optical path length L opt ( ⁇ ) of light 26 through prism 32 changes because of change in wavelength.
  • optical path length L opt ( ⁇ 0 ) is:
  • optical path length L opt ( ⁇ ) is:
  • ⁇ l is the difference in physical length as indicated in Fig 4.
  • light 26 at wavelength ⁇ 0 passes through a physical thickness t 0 in wedge filter 42 and through an optical thickness t at wavelength ⁇ .
  • the optical thicknesses are obtained by multiplying these physical thicknesses by index of refraction n w of wedge filter 42 at these respective wavelengths (i.e., at ⁇ 0 and ⁇ ) .
  • the new thickness t is a distance ⁇ d lower and is related to physical thickness t 0 as follows:
  • wavelength ⁇ to the original wavelength ⁇ 0 as follows:
  • apex angles Q X f ⁇ 2 are equal and the indices of refraction n l r n 2 of prisms 30, 32 are equal and have the same dependence on wavelength.
  • mode hop-free tuning behavior of laser 10 is achieved as follows. As stage 48 displaces prism 32 and wedge 42, pass band 54 of wedge filter 42 moves, as indicated in dotted lines. Simultaneously, mode 46j shifts in wavelength from operating wavelength ⁇ opl to -operating wavelength ⁇ op2 , as indicated in dashed lines. In fact, all modes 46 of light 26 shift continuously because prism 32 continuously compensates the optical path length L opt of cavity 20. The location of modes 46 after the displacement is denoted by primes for clarity.
  • cavity 20 continues to support mode 46j which remains centered in pass band 54 even as it migrates to its new position at 46j' and changes its operating wavelength from ⁇ opl to ⁇ op2 . Therefore, mode hops to other modes, e.g., adjacent modes 46i, 46k at different wavelengths are avoided at all times.
  • actuator 50 displaces stage 48 along directions other than that indicated by arrow S and/or one or both prisms 30, 32 are slightly rotated to prevent mode hops.
  • tunable laser 10 with external cavity 20 can be modified in many ways.
  • laser 10 may use a pair of prisms 80 as illustrated in Fig. 5.
  • Fig. 5 uses corresponding reference numbers to refer to corresponding parts.
  • a first prism 82 of prism pair 80 is designed in the same manner as first prism 30.
  • second prism 84 is designed like prism 32, but is integrated with a wedge filter 86 to eliminate the air gap between them.
  • a high reflection coating 88 is interposed between prism 84 and wedge filter 86 in order to ensure that wedge filter 86 operates to efficiently select the operating wavelength.
  • a second reflector 90 used in this embodiment is a high reflector consisting of a high reflection coating 92 deposited on a substrate 94. In this embodiment light 26 is not out- coupled through second reflector 90.
  • This embodiment is analogous to the preferred embodiment and has the advantage of integrating second prism 84 with wedge filter 86 to thus reduce the number of parts and the number of surfaces at which light 26 experiences losses.
  • Prism 84 is displaced along arrow S during wavelength tuning, but other movements of one or both prisms 82, 84 including rotation can be performed as well to prevent any eventual mode hops.
  • a prism pair 100 consists of a first prism 102 and a second prism 104. Pair of prisms 100 form a dispersion compensator, as in the previous embodiments, and prism 102 also acts as optical path length compensator. For this purpose, prism 102 is mounted on a stage 106.
  • prism pair 100 defines a gap filter 108 having a wedge angle between a first surface 110 of first prism 102 and a second surface 112 of second prism 104.
  • Gap filter 108 forms the wavelength selector in this embodiment.
  • the wedge angle can be made small enough to make gap filter 108 operate like a Fabry-Perot etalon.
  • first surface 110 and second surface 112 of prisms 102, 104 are provided with high reflectivity coatings 114, 116 to ensure sufficiently efficient filtering operation of gap filter 108.
  • surfaces 118, 120 with anti- reflection coatings 122, 124 to ensure that light 26 does not experience significant losses at surfaces 118, 120. This is important in this embodiment, because light 26 passes through surfaces 118, 120 of prisms 102, 104 at far from normal incidence and is thus more likely to be reflected rather than transmitted through surfaces 118, 120.
  • Prisms 102, 104 are oriented such that their external surfaces 118, 120 are maintained parallel during wavelength tuning which occurs as prism 102 is displaced along the direction indicated by arrow S on stage 106.
  • the relationship between wedge angle ⁇ and apex angle 0 ! of moving prism 102 is the same as the relationship between wedge angle and apex angle ⁇ 2 of the moving prism in the previous embodiments.
  • apex angles ⁇ l ⁇ 2 are preferably equal, the relationship is the same between wedge angle and apex angle ⁇ 2 of prism 104.
  • Stage 106 is preferably driven by an actuator 126 which can displace prism 102 along the direction of arrow S as well as rotate prism 102 together with prism 104 as indicated by arrow ⁇ .
  • actuator 126 can displace prism 102 along the direction of arrow S as well as rotate prism 102 together with prism 104 as indicated by arrow ⁇ .
  • Such rotation of prism pair 102, 104 is highly advantageous since it allows the operator to make fine adjustments of cavity length to ensure that mode-hops do not occur during wavelength tuning.
  • optical path length compensation and dispersion compensation are all performed by only prisms 102 and 104, this embodiment is very efficient in its use of parts. For these reasons the embodiment of Fig. 6 is preferred whenever high-precision actuator 126 capable of very precisely displacing and rotating prism pair 102, 104 is available.
  • FIG. 7 illustrates a laser 130 employing a coupler 132 for coupling out output light 134 and 136 from cavity 20.
  • Laser 130 is similar to laser 10 of Fig. 1 and corresponding parts are labeled with the same reference numbers.
  • Laser 130 has a high reflector 138 on facet 16 of medium 12 serving as the first reflector.
  • a low reflector 140 is provided on facet 14 of medium 12 to improve the lasing efficiency of medium 12.
  • a second reflector 142 is also a high reflector with a high reflectivity coating 144 deposited on a substrate 146.
  • output light 134, 136 is derived from cavity 20 only from coupler 132.
  • a laser 150 similar to laser 10 of Fig. 1 and using the same reference numbers to designate corresponding parts uses a polarizing beam splitter 152 to obtain output light 154 in an S-polarization 156.
  • facet 16 of medium 12 is provided with a high reflector 158 serving as the first reflector of cavity 20.
  • a second reflector 160 consisting of a high reflectivity coating 162 deposited on a substrate 164 delimits cavity 20 at the opposite end.
  • Facet 14 of medium 12 is provided with a polarizer 166 to ensure that light 26 emitted from medium 12 is contained in a P- polarization 168. Since polarizing beam splitter 152 is arranged to transmit P-polarization 168 it allows light 26 to continue propagating to the right.
  • a Faraday rotator 170 is positioned before prism pair 28.
  • the function of Faraday rotator 170 is to rotate P-polarization 168 slightly on each pass.
  • the polarization of light 26 is rotated by a certain small angle when propagating toward prism pair 28 and by the same angle when returning from prism pair 28.
  • the polarization of light 26 is slightly off the pure P-polarization.
  • light 26 approaching polarizing beam splitter 152 from the right has an S- polarization component.
  • polarizing beam splitter 152 deflects light 26 approaching from the right in S- polarization 156 out of cavity 20 in the form of output light 154.
  • a prism pair analogous to 82, 84 with integrated filter 86 can be substituted for prism pair 30, 32.
  • a prism pair defining a gap filter analogous to the one discussed in Fig. 6 can also be used in the embodiments of Figs . 7 and 8.
  • FIG. 9 Still another embodiment of a tunable external cavity laser 180 in accordance with the invention is illustrated in Fig. 9.
  • Laser 180 shares the same parts with laser 10 of Fig. 1, with the exception that first prism 30 is mounted on a moving stage 182 driven by a piezo-electric actuator 184.
  • Actuator 184 is designed to move stage 182 along an axis generally orthogonal to the axis of cavity 20 as indicated by arrow S' or other preferred directions in a way that the two prism surfaces 36 and 38 are parallel during the independent or synchronized movement of two prisms.
  • a control unit 186 is connected to actuator 184 to control its operation.
  • control unit 52 can be used to control the operation of both actuator 50 and actuator 184.
  • prism 30 is moved up and down to change the optical path length L opt of cavity 20 and aid in mode-hop control.
  • the movement of prism 30 can be effectuated in concert with the movement of prism 32.
  • prisms 30, 32 can be moved independently using independent control loops.
  • adjustment of the optical path length and mode hop control can be achieved with either closed or open loop control of the positions of prisms 30, 32.
  • FIG. 10 Yet another embodiment of a tunable external cavity laser 200 in accordance with the invention is illustrated in Fig. 10.
  • laser 200 employs a partially reflective coating
  • Partially reflective coating 202 exhibits a sufficiently high reflectivity to cause a desired amount of light 26 to undergo internal reflection at surface 36 and thus form output light 204.
  • the reflectivity of coating 202 should not be so high as to interfere with proper lasing action within cavity 20.
  • partially reflective coating 202 can also be used on surface 38 to outcouple light 26 through prism 32.
  • stage 48 would need to be re-designed to allow the outcoupled light to pass through.

Abstract

L'invention concerne un laser à cavité externe accordable équipé d'un compensateur de longueur du chemin optique permettant d'ajuster une longueur du chemin optique de la cavité, un sélecteur de longueur d'onde permettant de sélectionner une longueur d'onde de travail de la lumière dans un mode longitudinal unique et un compensateur de dispersion permettant de compenser une dispersion de la lumière. Afin d'obtenir un accord sans saut de mode, le laser présente un synchroniseur permettant de synchroniser le compensateur de longueur du chemin optique, le sélecteur de longueur d'onde et le compensateur de dispersion afin de maintenir la lumière dans le mode longitudinal unique sélectionné tandis que le sélecteur de longueur d'onde accorde la longueur d'onde de travail. Le laser fait appel à une paire de prismes et à un filtre en coin ou à un filtre à entrefer pour mettre en oeuvre les fonctions du compensateur de longueur du chemin optique, du sélecteur de longueur d'onde et du compensateur de dispersion.
PCT/US2003/037440 2002-12-06 2003-11-20 Laser a cavite externe a compensation de dispersion pour accord sans saut de mode WO2004054054A1 (fr)

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US10/313,624 2002-12-06
US10/313,624 US6940879B2 (en) 2002-12-06 2002-12-06 External cavity laser with dispersion compensation for mode-hop-free tuning

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RU2725639C2 (ru) * 2018-04-09 2020-07-03 Акционерное общество "Российская корпорация ракетно-космического приборостроения и информационных систем" (АО "Российские космические системы") Перестраиваемый диодный лазер с внешним резонатором

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US20040202223A1 (en) * 2003-04-08 2004-10-14 Eric Crosson External cavity laser having improved single mode operation
US7218443B2 (en) * 2003-02-25 2007-05-15 Toptica Photonics Ag Generation of tunable light pulses
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